BACKGROUND OF THE INVENTION
Field of the Invention
[0001] The present invention relates to a short-circuit distance relay for protecting a
single-channel power transmission system with power supplies installed at two ends
thereof, and more particularly to an improved distance relay which is capable of eliminating
a distance measurement error induced by a voltage drop component flowing through a
fault-point resistance from the remote-end power supply.
Description of the Prior Art
[0002] In the conventional short-circuit distance relays of this type known heretofore,
there have been existent some technical problems as described in "Handbook of Protective
Relays" (Ohm CO., Ltd., 2nd edition, 2nd printing, April 25, 1970, pp. 111 - 112);
"Protective Relay Technology" (Denki Shoin, 1st edition, 1st printing, October 15,
1972, pp. 323 - 324); "Protective Relays" (Albert Russell, 1st edition, 1969, pp.
270 - 274); and "Applied Protective Relaying" (Westinghouse Electric Corp., Copyright
1976, pp. 10 - 34, 10 - 42 & 10 - 44). In the present stage of development, however,
such problems have not been solved yet. An exemplary conventional apparatus will now
be described below.
[0003] Fig. 1 is a block diagram of a single-channel power transmission system with power
supplies installed at two ends thereof, wherein there are shown a local-end power
supply 1, a voltage transformer 2, a bus 3, a voltage transformer 4, a current transformer
5, a short-circuit distance relay 6, a power transmission line 7, a fault point 8,
a bus 9, a voltage transformer 10, and a remote-end power supply 11.
[0004] Fig. 2 is an equivalent circuit diagram representing occurrence of a two-line short-circuit
fault at the point 8 in Fig. 1. In the figure, there are shown a fault-phase supply
voltage EΔP at the local end (P), a fault-phase supply voltage EΔQ at the remote end
(Q), an impedance ZgP behind the local end, an impedance ZgQ behind the remote end,
an impedance Z per unit length (km) of the power transmission line, a distance X (km)
from the short-circuit distance relay to the fault point, an entire length L of the
power transmission line, a fault-point resistance RF, a voltage VR at the location
of the short-circuit distance relay, a fault current IP flowing through the fault
point from the local-end power supply, and a fault current IQ flowing through the
fault point from the remote-end power supply.
[0005] In Fig. 2, the voltage VR at the location of the short-circuit distance relay 6 is
given by Eq. (1) below.

[0006] On the basis of the current IP flowing in the short-circuit distance relay 6, the
impedance measured by the relay 6 is obtained through division of the voltage VR,
which is applied to the relay 6, by the current IP as follows.

When the fault-point resistance RF is zero in Eq. (2), the impedance to be measured
is obtainable as XZ in which Z represents the impedance per unit length of the transmission
line 7, so that it is possible to measure the distance from the location of the short-circuit
distance relay 6 to the fault point 8. Also in case the fault-point resistance RF
has a finite value instead of being zero, the above distance is measurable from the
sinusoidal component of the voltage VR relative to the fault current IP if an in-phase
relationship is existent without any phase difference between the fault current IP
from the local-end power supply 1 and the fault current IQ from the remote-end power
supply despite a variation of the second-term resistance component in Eq. (2). This
is obvious as the reactance component of XZ remains unchanged.
[0007] Fig. 3 graphically shows an exemplary case with occurrence of a fault in a conventional
short-circuit distance relay 6, wherein R-jx coordinates represent a vector obtained
when the fault current IQ from the remote terminal has a phase lag in comparison with
the fault current IP at the local end.
[0008] In the graph of Fig. 3, there are plotted a voltage drop XZIP (segment OB) up to
the fault point 8 (in Fig. 1) on the power transmission line 7 (in Fig. 1); a , voltage
drop RFIP (segment BC) caused across the fault-point resistance RF by the local-end
current; a voltage drop RFIQ (segment CD) caused across the fault-point resistance
RF by the remote-end current; an impedance angle a of the power transmission line;
a phase difference angle 6 between the voltage VR and the current IP at the relay
location; and a phase difference angle 6 between the local-end current IP and the
remote-end current IQ.
[0009] In the conventional short-circuit distance relay having the above-mentioned constitution,
the voltage VR at the relay location is represented by a segment OD of Fig. 3 from
Eq. (1) when there exists a phase difference angle between the local-end current and
the remote-end current, so that the reactance component obtained from the sinusoidal
component of the voltage VR relative to the local-end current IP becomes equal to
the value at the occurrence of a fault with the fault-point resistance RF being zero
at a point A on the power transmission line, whereby the point A comes to vary depending
on the fault-point resistance RF, the ratio between the local-end current IP and the
remote-end current IQ, and also on the phase difference angle 6 between the local-end
current IP and the remote-end current IQ. Thus, it has been unavoidable heretofore
that an error is induced in measuring the distance up to the fault point.
SUMMARY OF THE INVENTION
[0010] The present invention has been accomplished in view of the afore-mentioned disadvantages
observed in the prior art. And its object resides in providing an improved short-circuit
distance relay which is capable of eliminating an error in measurement of the distance
from the information including a positive-phase voltage and a positive-phase current
in a normal state of a power transmission system, and also a positive-phase voltage,
a positive-phase current and a negative-phase current in a faulty state of the system.
[0011] An exemplary embodiment of the present invention comprises a plurality of means for
deriving a positive- .phase voltage V and a positive-phase current IL in a normal
state of a power transmission system, and also a positive-phase voltage VF, a positive-phase
current IF and a negative-phase current I2 in a faulty state of the system; integrating
means consisting of a sixth arithmetic circuit for computing I2 · (VF - V) from the
outputs of the deriving means, a seventh arithmetic circuit for computing I2 · (IF
- IL)-(ZP + ZQ) from the outputs of the deriving means also from a positive-phase
impedance (ZP + ZQ) of the system, an eighth arithmetic circuit for computing (IF
- IL)
2·(LZ2 + ZQ2) from a negative-phase impedance (LZ2 + ZQ2) in the direction toward the
remote end as viewed from the relay location, and a ninth arithmetic circuit for.
computing (IF - IL) - (I2 - IF + IL); and means for calculating the impedance up to
.the fault point from the output of the integrating means, whereby the fault-point
resistance RF is rendered unconcerned with the distance measurement.
BRIEF DESCRIPTION OF THE DRAWINGS
[0012] Fig. 1 is a block diagram of a single-channel power transmission system with power
supplies installed at two ends thereof; Fig. 2 is an equivalent circuit diagram in
an exemplary case with occurrence of a two-line short-circuit fault in Fig. 1; Fig.
3 is a vector diagram showing that a disadvantage is existent in a conventional short-circuit
distance relay; Fig. 4 is a circuit diagram showing symmetrical components at the
occurrence of a two-line short-circuit fault in Fig. 1: Fig. 5 is a circuit diagram
showing a current distribution at the occurrence of a fault in Fig. 4; and Fig. 6
is a circuit diagram of an exemplary short-circuit distance relay embodying the present
invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0013] Hereinafter an exemplary embodiment of the present invention will be described with
reference to the accompanying drawings.
[0014] In the circuit diagram of Fig. 4 showing symmetrical components at the occurrence
of a two-line short-circuit fault at the point 8 in Fig. 1, there are included a positive-phase
circuit 21, a negative-phase circuit 22, a switch 23 simulating a portion where a
two-line short-circuit fault is induced, positive-phase circuits 31 and 32 in the
bus 3 of Fig. 1, a negative-phase circuit 32 in the bus 3, current transformers 51
and 52 for deriving a positive-phase current and a negative-phase current at the position
of the current transformer 5 shown in Fig. 1, a positive-phase circuit 91 in the bus
of Fig. 1, and a negative-phase circuit 92 in the bus of Fig. 1. Further shown in
Fig. 4 are a local-end supply voltage EP, a remote-end supply voltage EQ, a positive-phase
impedance ZP1 behind the local end, a negative-phase impedance ZP2 behind the local
end, a positive-phase impedance Zl per unit length (km) of the power transmission
line, a negative-phase impedance Z2 per unit length (km) of the power transmission
line, a distance X (km) from the relay location to a fault point, an entire length
L (km) of the power transmission line, a positive-phase impedance ZQ1 behind the remote
end, a negative-phase impedance ZQ2 behind the remote end, a fault-point resistance
RF, a positive-phase voltage V at the relay location in a normal state of the system,
a positive-phase current IL flowing through the relay location in a normal state of
the system (when the switch 23 is open), a positive-phase current I2 flowing through
the relay location in a faulty state of the system (when the switch 23 is closed),
a negative-phase current 12 flowing through the relay location in a faulty state of
the system (when the switch 23 is closed), a current IF1 flowing through the fault
point, and a composite impedance ZF constituted of the negative-phase circuit impedance
and the fault-point resistance.
[0015] Fig. 5 shows a distribution of the fault current in Fig. 4.
[0016] In Fig. 5(a), ZF denotes a combination of the negative-phase circuit impedance and
the fault-point resistance RF in Fig. 4, indicating that the system is in a normal
state where the fault switch 23 is open. In such a normal state, a current IL flows
in the current transformer 51 with a positive-phase voltage V being applied to the
bus 31.
[0017] Fig. 5(b) shows a faulty state of the system where the fault switch 23 is closed
from its open position in Fig. 5(a). In such a faulty state, a current IF flows in
the current transformer 51 with a positive-phase voltage VF being applied to the bus
31, and a fault current IF1 flows in the switch 23 simulating the fault point.
[0018] In Fig. 5(c), supply voltages EP and EQ at the two ends are removed, and an additional
power supply e is provided at the fault point in such a manner that the current IF1
flowing through the fault point becomes opposite in polarity to that shown in Fig.
5(b).
[0019] Since the current flowing in the fault-point simulating switch 23 becomes zero as
a result of mutual superposition of Figs. 5(b) and 5(c), it follows that the configuration
of Fig. 5(a) is achieved by superposing Fig. 5(c) on Fig. 5(b).
[0020] This is manifest from the Ho-Thevenin's theorem.
[0021] Due to the power supply e provided in the example of Fig. 5(c), a current Ia comes
to flow in the current transformer 51, so that

[0022] The value of Iα can be calculated as follows.

where ZP = ZP1 + XZ1

[0023] According to Fig. 5(a),

[0024] Therefore, from Eqs. (3) through (5),

[0025] Further according to Fig. 5(a),

[0026] From Eqs. (6) and (7),

[0027] The value of IF1 in Eq. (8) can be calculated in the manner described below. First,
Eq. (9) is obtained according to the negative-phase circuit shown in Fig. 4.

[0028] Solving the above with respect to IF1,

[0029] Substituting Eq. (10) in Eq. (8),

[0030] Substituting Eq. (5) in Eq. (11),

[0031] Rewriting Eq. (12) with respect to XZ1,

where ZT2 = ZP2 + LZ2 + ZQ2
[0032] From Eq. (4), ZP + ZQ in Eq. (13) is equal to ZP1+LZ1+ZQ1, and the impedance of the
positive-phase circuit is generally equal to that of the negative-phase circuit. Therefore,
it is possible to rewrite the above as ZP + ZQ = ZT2 and Zl = Z2, so that Eq. (13)
can be simplified as

where the entire values are known with the exception of the supply voltage EQ at the
remote end.
[0033] The supply voltage EQ at the remote end can be calculated in the following manner.
First, from the circuit of Fig. 5(a) in a normal state of the system,

[0034] Also from the circuit of Fig. 5(b) in a faulty state of the system,

[0035] Accordingly, from Eqs. (15) and (16),

[0036] Substituting EP in Eq. (17) in Eq. (5),

[0037] The impedance up to the fault point is obtained from .Eq. (19) by substituting Eq.
(18) for Eq. (14).

[0038] Fig. 6 is a circuit diagram of an exemplary -distance relay embodying the present
invention, wherein there are shown an input terminal 101 for a positive-phase voltage
component, an input terminal 102 for a positive-phase current component, an input
terminal 103 for a negative-phase current component, a selector switch 104 actuated
in response to the output of a fault detector (not shown), a first memory circuit
105, a second memory circuit 106, arithmetic circuits 107 - 110 - (integrating means),
an adder circuit 111 and a divider circuit 112 (impedance calculating means), and
an output terminal 113.
[0039] In the circuit configuration mentioned above, the relay performs the following operation.
[0040] The selector switch 104 responsive to the output of a fault detector (not shown)
is so arranged that its - lower contact 104a is connected in a faulty.state of the
power transmission system as illustrated in Fig. 6 and its upper contact 104b is connected
in a normal state of the system. Consequently, in the memory circuit 105 are stored
both the positive-phase voltage V applied via the input terminal 101 in a normal state
of the system and the positive-phase voltage VF in a faulty state thereof.
[0041] In the memory circuit 106 are stored both the positive-phase current IL applied via
the input terminal 102 in a normal state of the system and the positive-phase current
IF in a faulty state thereof.
[0042] In the sixth arithmetic circuit 107, I2·(VF-V) is computed from the outputs of the
memory circuits 105 and 106 and also from the negative-phase current component introduced
via the input terminal 103. In the seventh arithmetic circuit 108, 12
'(IF - IL)· (ZP + ZQ) is computed from the output of the memory circuit 106, the component
introduced via the input terminal 103 and also from the sum of the positive impedances
(ZP + ZQ) of the system. In the eighth arithmetic circuit 109, (IF - IL)
2·(LZ2 + ZQ2) is computed from the output of the memory circuit 106 and the sum of
the negative-phase impedances (LZ2 + ZQ2) in the direction toward the remote end as
viewed from the relay location. And further in the ninth arithmetic circuit 110, (IF
- IL)(I2 - IF + IL) is computed from the output of the memory circuit 106 and the
component introduced via the input terminal 103.
[0043] The adder circuit 111 executes a calculation by first adding the outputs of the arithmetic
circuits 107 and 108 and then subtracting the output of the eighth arithmetic circuit
109 from the sum thus obtained. Subsequently, the divider circuit 112 in the next
stage divides the output of the adder circuit 111 by the output of the ninth arithmetic
circuit 110 to calculate the impedance of Eq. (19) up to the fault point and then
provides the result at the output terminal 113.
[0044] As described hereinabove, according to the short-circuit distance relay of the present
invention, the impedance up to the fault point is computed from the information including
the positive-phase voltage'V and the positive-phase current IL in a normal state of
the power transmission system and also the positive-phase voltage VF, the positive-phase
current IF and the negative-phase current I2 in a faulty state of the system, so that
the fault-point resistance RF is rendered unconcerned with the impedance. Thus, it
becomes possible to eliminate any error induced in the prior art during measurement
of the distance by the voltage drop caused across the fault-point resistance RF due
to the phase difference between the two power supplies at the system ends.
[0045] In order to simplify the description relative to the foregoing embodiment, the computation
in the above-mentioned equations is executed by utilizing the equality of the impedances
of the positive-phase circuit and the negative-phase circuit. However, it is a matter
of course that such computation may be carried out on the basis that the two impedances
are not equal to each other.
[0046] As described hereinabove, according to the present invention which is so constituted
as to compute the impedance up to the fault point from the circuit constants of the
power transmission system and the information including the currents and voltages
in both a normal state and a faulty state of the system, remarkable advantages are
attainable in accomplishing a high-reliability short-circuit distance relay capable
of substantially eliminating any error induced in the distance measurement by the
resistance at the fault point.